Data-driven CFD scaling of bioinspired Mars flight vehicles for hover
Introduction
Improved information about the Martian environment will reduce uncertainties and risks in future exploration, including human missions. Aerial vehicles can perform sensing and other tasks that fill the gaps in the information gathering capabilities of Mars orbiters and land-based rovers. Flight vehicles capable of near-surface hovering are attractive candidates for such information gathering missions. These missions may include surveying remote locations, retrieving samples, efficiently generating topographic models of the surrounding terrain, providing near-surface weather data, and assisting rovers in path planning. In addition, the recent advancements in swarming flight and autonomy offer additional design options and possibly improved efficiencies for these missions [1].
Though the atmospheric viscosity on Mars is similar to that of Earth, μMars = 0.83μEarth [2], the ultra-low density atmospheric environment has proved a difficult challenge in designing realizable Martian flight vehicles. Despite the gravitational acceleration on Mars requiring less lift production than on Earth for a given vehicle mass, where gMars = 0.38gEarth, the reduced density on Mars compared to Earth being ρMars = 0.0142ρEarth can be quite prohibitive for generating sufficient aerodynamic forces to fly using conventional designs [3]. Although NASA is sending the helicopter Ingenuity to Mars during the 2020 Perseverance rover mission, such a solution results in a design that is relatively large (around 1.8 kg vehicle with a 1.21 m rotor diameter) [4] and potentially less aerodynamically efficient when operated at the low Reynolds numbers inherent to Martian flight [5].
Bioinspired flapping wing solutions can overcome the difficulties associated with flight in the rarefied Martian atmosphere [6]. The thin Martian atmosphere results in a relatively low Reynolds number Re which is directly proportional to the fluid density ρ. Insects make use of efficient, unsteady aerodynamic mechanisms that occur at low Reynolds numbers. These mechanisms include delayed stall via an attached leading-edge vortex (LEV), wake capture, and enhanced circulation via rotational lift [7,8]. As such, properly scaled flapping wing motion on Mars has been demonstrated to exhibit the same mechanisms and potential for flight [6,9].
The method used to achieve these bioinspired solutions on Mars is based on the well-established fluid dynamics concept of dynamic similarity [10,11]. In general, to dynamically scale a system in the context of fluid dynamics is to preserve the geometrical shape but change the relevant dimensional parameters (e.g. fluid density, viscosity, wing velocity, etc.) such that the set of governing dimensionless parameters (e.g. Reynolds number, lift coefficient, etc.) is preserved between the two configurations. For example, dynamic similarity guides the scaling of model aircraft for sub-scale wind tunnel tests before full-scale flight tests are performed. Not only does dynamic similarity allow for convenient physical scaling of the system, it also reduces the total number of parameters required to fully describe a system involving multiple parameters, thus reducing the design space to a more manageable set of parameters [12].
Our previous bioinspired solutions [6] are dynamically similar to terrestrial insects' flapping wing motions, and take advantage of similar unsteady, high lift coefficient producing mechanisms on Mars. The relevant set of dimensionless parameters for a rigid flapping wing are: aspect ratio AR, related to the slenderness of a wing; Reynolds number Re, the ratio between the flow inertia and viscous forces; reduced frequency k, a measure of flow unsteadiness; Mach number M, related to the flow compressibility; and pitch amplitude A, measuring the wing's angle of attack. To maintain dynamic similarity with insects on Earth, these parameters were kept in the insect-inspired flight regime. Starting from the morphological parameters corresponding to a bumblebee, the wings were uniformly scaled to approximately the size of cicada wings. The flapping frequency was also reduced to 63 Hz, approximately 43% that of a bumblebee (~155 Hz). Generating such a solution through biomimicry not only provides a means of producing sufficient lift, but it also results in a flight vehicle that has the potential to benefit from other attractive qualities of insect flight such as hovering, high maneuverability, long range/endurance flight, and high payload capacity. To exploit the advantages of insect-inspired flight, we extended the study to quantify the payload margin of the bumblebee-inspired flapping wing micro air vehicle (FWMAV) and determined that it can carry a payload on the order of its own body weight [13]. It was determined that the payload capabilities are limited by maintaining dynamically similar motion.
While successful flapping wing flight on Mars has been simulated [6,9], these results were limited to vehicle masses that were less than 1 g, operated at Reynolds numbers of less than 200, and reduced frequencies between 0.2 and 0.35. The general scaling range between viable insect-inspired flapping wing vehicles and infeasible designs is currently unknown.
This paper seeks to identify the physical solution range for bioinspired flapping wing flight on Mars. We present a data-driven CFD scaling model that accounts for nonlinearities in the mean lift based on the relevant dimensionless parameters. Using this method, we generate hover solutions for flapping wing vehicles on Mars that range from 1 g to 1 kg. We verify these bioinspired solutions using a well-validated 3D Navier-Stokes equation solver. Furthermore, we investigate the resulting dimensional design space to understand the trends and limits of scaling a bioinspired flapping wing vehicle for flight on Mars. Our previous solution at the insect scale [13] had a mass of 0.2 g. Current Earth-based flapping wing robots have masses of O(100–101) grams. These include Chiba University's bioinspired MAV (6 g) [14], the DelFly II (16 g) [15], the Nano Hummingbird (19 g) [16], the KUBeetle-S (16 g) [17,18], and various other FWMAV prototypes (6 and 12 g) [19]. Additionally, the Mars helicopter Ingenuity mass is O(103) grams [4]. While insect size micro-air vehicles can employ stealth, larger vehicles with increased payload capability can be more beneficial for Mars exploration since they can carry larger sensors than insect-size vehicles. We provide a method for generating dynamically similar hovering design solutions for Martian flapping wing robots with total masses on the order of the current Earth FWMAVs, as well as the Mars helicopter Ingenuity.
Section snippets
Methodology
The approach to finding a bioinspired solution builds on methodology from our past studies [6,13]. We originally used a trimming algorithm to modify the kinematics such that the lift balances the weight in dynamical equilibrium. Here we develop a general methodology to scale the wing size and kinematics to achieve a lift force that balances the vehicle weight on Mars in an averaged sense. We first determine a dynamically similar solution based on the desired vehicle mass by using a scaling
Family of solutions for Mars flapping wing robots of various masses
The scaling method can be used to determine a family of solutions for dynamically similar flapping wing motion on Mars for vehicles of various masses. The approach described in Section 2.4 is applied for a range of masses m, allowing the relationships between the aspect ratio, Reynolds number, and kinematics to be investigated. We consider three discrete aspect ratios: AR = 2, 4, and 6 to cover the range of insect-inspired values. The reduced frequency values are in the insect flight regime,
Concluding remarks
This study builds on our prior work of achieving hovering flight on Mars using bioinspired flapping wing motion based on a bumblebee with enlarged wings [6]. Using the present scaling method which leverages a 3D Navier-Stokes trained neural network model, approximate wing size properties and kinematics are determined such that sufficient lift is generated to achieve hover on Mars. This method was confirmed by 3D Navier-Stokes solutions for vehicles that varied from 1 g to 1 kg and had a broad
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgments
This work was in part supported by the NASA Innovative Advanced Concepts program under the grant 80NSSC18K0870 and partly by the University of Alabama in Huntsville through supplemental research funding. Jeremy Pohly is supported by the NASA/Alabama Space Grant Consortium, NASA Training Grant NNX15AJ18H.
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